Signaltonoise ratio (SNR or S/N) is a measure used in science and engineering that compares the level of a desired signal to the level of background noise. SNR is defined as the ratio of signal power to noise power, often expressed in decibels. A ratio higher than 1:1 (greater than 0 dB) indicates more signal than noise.
SNR is an important parameter that affects the performance and quality of systems that process or transmit signals, such as communication systems, audio systems, radar systems, imaging systems, and data acquisition systems. A high SNR means that the signal is clear and easy to detect or interpret, while a low SNR means that the signal is corrupted or obscured by noise and may be difficult to distinguish or recover. SNR can be improved by various methods, such as increasing the signal strength, reducing the noise level, filtering out unwanted noise, or using error correction techniques.
SNR also determines the maximum possible amount of data that can be transmitted reliably over a given channel, which depends on its bandwidth and SNR. This relationship is described by the Shannon–Hartley theorem, which is a fundamental law of information theory.
SNR can be calculated using different formulas depending on how the signal and noise are measured and defined. The most common way to express SNR is in decibels, which is a logarithmic scale that makes it easier to compare large or small values. Other definitions of SNR may use different factors or bases for the logarithm, depending on the context and application.
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Transcription
Definition
Signaltonoise ratio is defined as the ratio of the power of a signal (meaningful input) to the power of background noise (meaningless or unwanted input):
where P is average power. Both signal and noise power must be measured at the same or equivalent points in a system, and within the same system bandwidth.
Depending on whether the signal is a constant (s) or a random variable (S), the signaltonoise ratio for random noise N becomes:^{[1]}
where E refers to the expected value, i.e. in this case the mean square of N, or
If the noise has expected value of zero, as is common, the denominator is its variance, the square of its standard deviation σ_{N}.
The signal and the noise must be measured the same way, for example as voltages across the same impedance. The root mean squares can alternatively be used in the ratio:
where A is root mean square (RMS) amplitude (for example, RMS voltage).
Decibels
Because many signals have a very wide dynamic range, signals are often expressed using the logarithmic decibel scale. Based upon the definition of decibel, signal and noise may be expressed in decibels (dB) as
and
In a similar manner, SNR may be expressed in decibels as
Using the definition of SNR
Using the quotient rule for logarithms
Substituting the definitions of SNR, signal, and noise in decibels into the above equation results in an important formula for calculating the signal to noise ratio in decibels, when the signal and noise are also in decibels:
In the above formula, P is measured in units of power, such as watts (W) or milliwatts (mW), and the signaltonoise ratio is a pure number.
However, when the signal and noise are measured in volts (V) or amperes (A), which are measures of amplitude,^{[note 1]} they must first be squared to obtain a quantity proportional to power, as shown below:
Dynamic range
The concepts of signaltonoise ratio and dynamic range are closely related. Dynamic range measures the ratio between the strongest undistorted signal on a channel and the minimum discernible signal, which for most purposes is the noise level. SNR measures the ratio between an arbitrary signal level (not necessarily the most powerful signal possible) and noise. Measuring signaltonoise ratios requires the selection of a representative or reference signal. In audio engineering, the reference signal is usually a sine wave at a standardized nominal or alignment level, such as 1 kHz at +4 dBu (1.228 V_{RMS}).
SNR is usually taken to indicate an average signaltonoise ratio, as it is possible that instantaneous signaltonoise ratios will be considerably different. The concept can be understood as normalizing the noise level to 1 (0 dB) and measuring how far the signal 'stands out'.
Difference from conventional power
In physics, the average power of an AC signal is defined as the average value of voltage times current; for resistive (nonreactive) circuits, where voltage and current are in phase, this is equivalent to the product of the rms voltage and current:
But in signal processing and communication, one usually assumes that ^{[3]} so that factor is usually not included while measuring power or energy of a signal. This may cause some confusion among readers, but the resistance factor is not significant for typical operations performed in signal processing, or for computing power ratios. For most cases, the power of a signal would be considered to be simply
Alternative definition
An alternative definition of SNR is as the reciprocal of the coefficient of variation, i.e., the ratio of mean to standard deviation of a signal or measurement:^{[4]}^{[5]}
where is the signal mean or expected value and is the standard deviation of the noise, or an estimate thereof.^{[note 2]} Notice that such an alternative definition is only useful for variables that are always nonnegative (such as photon counts and luminance), and it is only an approximation since . It is commonly used in image processing,^{[6]}^{[7]}^{[8]}^{[9]} where the SNR of an image is usually calculated as the ratio of the mean pixel value to the standard deviation of the pixel values over a given neighborhood.
Sometimes^{[further explanation needed]} SNR is defined as the square of the alternative definition above, in which case it is equivalent to the more common definition:
This definition is closely related to the sensitivity index or d', when assuming that the signal has two states separated by signal amplitude , and the noise standard deviation does not change between the two states.
The Rose criterion (named after Albert Rose) states that an SNR of at least 5 is needed to be able to distinguish image features with certainty. An SNR less than 5 means less than 100% certainty in identifying image details.^{[5]}^{[10]}
Yet another alternative, very specific, and distinct definition of SNR is employed to characterize sensitivity of imaging systems; see Signaltonoise ratio (imaging).
Related measures are the "contrast ratio" and the "contrasttonoise ratio".
Modulation system measurements
Amplitude modulation
Channel signaltonoise ratio is given by
where W is the bandwidth and is modulation index
Output signaltonoise ratio (of AM receiver) is given by
Frequency modulation
Channel signaltonoise ratio is given by
Output signaltonoise ratio is given by
Noise reduction
All real measurements are disturbed by noise. This includes electronic noise, but can also include external events that affect the measured phenomenon — wind, vibrations, the gravitational attraction of the moon, variations of temperature, variations of humidity, etc., depending on what is measured and of the sensitivity of the device. It is often possible to reduce the noise by controlling the environment.
Internal electronic noise of measurement systems can be reduced through the use of lownoise amplifiers.
When the characteristics of the noise are known and are different from the signal, it is possible to use a filter to reduce the noise. For example, a lockin amplifier can extract a narrow bandwidth signal from broadband noise a million times stronger.
When the signal is constant or periodic and the noise is random, it is possible to enhance the SNR by averaging the measurements. In this case the noise goes down as the square root of the number of averaged samples.
Digital signals
When a measurement is digitized, the number of bits used to represent the measurement determines the maximum possible signaltonoise ratio. This is because the minimum possible noise level is the error caused by the quantization of the signal, sometimes called quantization noise. This noise level is nonlinear and signaldependent; different calculations exist for different signal models. Quantization noise is modeled as an analog error signal summed with the signal before quantization ("additive noise").
This theoretical maximum SNR assumes a perfect input signal. If the input signal is already noisy (as is usually the case), the signal's noise may be larger than the quantization noise. Real analogtodigital converters also have other sources of noise that further decrease the SNR compared to the theoretical maximum from the idealized quantization noise, including the intentional addition of dither.
Although noise levels in a digital system can be expressed using SNR, it is more common to use E_{b}/N_{o}, the energy per bit per noise power spectral density.
The modulation error ratio (MER) is a measure of the SNR in a digitally modulated signal.
Fixed point
For nbit integers with equal distance between quantization levels (uniform quantization) the dynamic range (DR) is also determined.
Assuming a uniform distribution of input signal values, the quantization noise is a uniformly distributed random signal with a peaktopeak amplitude of one quantization level, making the amplitude ratio 2^{n}/1. The formula is then:
This relationship is the origin of statements like "16bit audio has a dynamic range of 96 dB". Each extra quantization bit increases the dynamic range by roughly 6 dB.
Assuming a fullscale sine wave signal (that is, the quantizer is designed such that it has the same minimum and maximum values as the input signal), the quantization noise approximates a sawtooth wave with peaktopeak amplitude of one quantization level^{[11]} and uniform distribution. In this case, the SNR is approximately
Floating point
Floatingpoint numbers provide a way to trade off signaltonoise ratio for an increase in dynamic range. For n bit floatingpoint numbers, with nm bits in the mantissa and m bits in the exponent:
Note that the dynamic range is much larger than fixedpoint, but at a cost of a worse signaltonoise ratio. This makes floatingpoint preferable in situations where the dynamic range is large or unpredictable. Fixedpoint's simpler implementations can be used with no signal quality disadvantage in systems where dynamic range is less than 6.02m. The very large dynamic range of floatingpoint can be a disadvantage, since it requires more forethought in designing algorithms.^{[12]}^{[note 3]}^{[note 4]}
Optical signals
Optical signals have a carrier frequency (about 200 THz and more) that is much higher than the modulation frequency. This way the noise covers a bandwidth that is much wider than the signal itself. The resulting signal influence relies mainly on the filtering of the noise. To describe the signal quality without taking the receiver into account, the optical SNR (OSNR) is used. The OSNR is the ratio between the signal power and the noise power in a given bandwidth. Most commonly a reference bandwidth of 0.1 nm is used. This bandwidth is independent of the modulation format, the frequency and the receiver. For instance an OSNR of 20 dB/0.1 nm could be given, even the signal of 40 GBit DPSK would not fit in this bandwidth. OSNR is measured with an optical spectrum analyzer.
Types and abbreviations
Signal to noise ratio may be abbreviated as SNR and less commonly as S/N. PSNR stands for peak signaltonoise ratio. GSNR stands for geometric signaltonoise ratio.^{[citation needed]} SINR is the signaltointerferenceplusnoise ratio.
Other uses
While SNR is commonly quoted for electrical signals, it can be applied to any form of signal, for example isotope levels in an ice core, biochemical signaling between cells, or financial trading signals. The term is sometimes used metaphorically to refer to the ratio of useful information to false or irrelevant data in a conversation or exchange. For example, in online discussion forums and other online communities, offtopic posts and spam are regarded as noise that interferes with the signal of appropriate discussion.^{[13]}
See also
Notes
 ^ The connection between optical power and voltage in an imaging system is linear. This usually means that the SNR of the electrical signal is calculated by the 10 log rule. With an interferometric system, however, where interest lies in the signal from one arm only, the field of the electromagnetic wave is proportional to the voltage (assuming that the intensity in the second, the reference arm is constant). Therefore the optical power of the measurement arm is directly proportional to the electrical power and electrical signals from optical interferometry are following the 20 log rule.^{[2]}
 ^ The exact methods may vary between fields. For example, if the signal data are known to be constant, then can be calculated using the standard deviation of the signal. If the signal data are not constant, then can be calculated from data where the signal is zero or relatively constant.
 ^ Often special filters are used to weight the noise: DINA, DINB, DINC, DIND, CCIR601; for video, special filters such as comb filters may be used.
 ^ Maximum possible full scale signal can be charged as peaktopeak or as RMS. Audio uses RMS, Video PP, which gave +9 dB more SNR for video.
References
 ^ Charles Sherman; John Butler (2007). Transducers and Arrays for Underwater Sound. Springer Science & Business Media. p. 276. ISBN 9780387331393.
 ^ Michael A. Choma, Marinko V. Sarunic, Changhuei Yang, Joseph A. Izatt. Sensitivity advantage of swept source and Fourier domain optical coherence tomography. Optics Express, 11(18). Sept 2003.
 ^ Gabriel L. A. de Sousa; George C. Cardoso (18 June 2018). "A batteryresistor analogy for further insights on measurement uncertainties". Physics Education. IOP Publishing. 53 (5): 055001. arXiv:1611.03425. Bibcode:2018PhyEd..53e5001D. doi:10.1088/13616552/aac84b. S2CID 125414987. Retrieved 5 May 2021.
 ^ D. J. Schroeder (1999). Astronomical optics (2nd ed.). Academic Press. p. 278. ISBN 9780126298109., p.278
 ^ ^{a} ^{b} Bushberg, J. T., et al., The Essential Physics of Medical Imaging, (2e). Philadelphia: Lippincott Williams & Wilkins, 2006, p. 280.
 ^ Rafael C. González, Richard Eugene Woods (2008). Digital image processing. Prentice Hall. p. 354. ISBN 9780131687288.
 ^ Tania Stathaki (2008). Image fusion: algorithms and applications. Academic Press. p. 471. ISBN 9780123725295.
 ^ Jitendra R. Raol (2009). MultiSensor Data Fusion: Theory and Practice. CRC Press. ISBN 9781439800034.
 ^ John C. Russ (2007). The image processing handbook. CRC Press. ISBN 9780849372544.
 ^
Rose, Albert (1973). Vision – Human and Electronic. Plenum Press. p. 10. ISBN 9780306307324.
[...] to reduce the number of false alarms to below unity, we will need [...] a signal whose amplitude is 4–5 times larger than the rms noise.
 ^ Defining and Testing Dynamic Parameters in HighSpeed ADCs — Maxim Integrated Products Application note 728
 ^ FixedPoint vs. FloatingPoint DSP for Superior Audio — Rane Corporation technical library
 ^ Breeding, Andy (2004). The Music Internet Untangled: Using Online Services to Expand Your Musical Horizons. Giant Path. p. 128. ISBN 9781932340020.
External links
 Walt Kester, Taking the Mystery out of the Infamous Formula,"SNR = 6.02N + 1.76dB," and Why You Should Care (PDF), Analog Devices, archived (PDF) from the original on 20221009, retrieved 20190410
 ADC and DAC Glossary – Maxim Integrated Products
 Understand SINAD, ENOB, SNR, THD, THD + N, and SFDR so you don't get lost in the noise floor – Analog Devices
 The Relationship of dynamic range to data word size in digital audio processing
 Calculation of signaltonoise ratio, noise voltage, and noise level
 Learning by simulations – a simulation showing the improvement of the SNR by time averaging
 Dynamic Performance Testing of Digital Audio D/A Converters
 Fundamental theorem of analog circuits: a minimum level of power must be dissipated to maintain a level of SNR
 Interactive webdemo of visualization of SNR in a QAM constellation diagram Institute of Telecommunicatons, University of Stuttgart
 Bernard Widrow,István Kollár (20080703), Quantization Noise: Roundoff Error in Digital Computation, Signal Processing, Control, and Communications, Cambridge University Press, Cambridge, UK, 2008. 778 p., ISBN 9780521886710
 Quantization Noise Widrow & Kollár Quantization book page with sample chapters and additional material
 Signaltonoise ratio online audio demonstrator  Virtual Communications Lab